In order to dynamically generate this asymmetry, the three Sakharov
conditions must be fulfilled [1]}: baryon number violation, \(C\)  and \(CP\)  violation and
departure from thermal equilibrium. In a type I seesaw scenario, a lepton
asymmetry \(Y_{L}\)  is generated
through the out-of-equilibrium \(CP\)  violating decays of \(N_{i}^{c}\)  that is
partially converted into the baryon asymmetry \(Y_{B}\)  via
sphaleron processes [2]}. In order to estimate the value of \(Y_{B}\) , we
perform our study in the case of unflavored leptogenesis due to the fact
that all RHN masses are above \(T=10^{12}(1+\tan ^{2}\beta )\)  as
discussed in [3]}. Moreover, since the RHN mass spectrum is not strongly hierarchical, we
consider the contributions of all three RHNs to the generation of
the BAU; \(Y_{B}=\sum \limits _{i=1}^{3}Y_{Bi}\)  with
\(Y_{Bi}\approx -1.266\times 10^{-3}\varepsilon _{N_{i}}\eta _{ii} \) 
